nuclear data for radiation therapy...nirs / himac 2 résumé introduction radiations used for...
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NIRS / HIMACNIRS / HIMAC
Nuclear Datafor
Radiation Therapy
Naruhiro Matsufuji, Yuki Kase and Tatsuaki KanaiNational Institute of Radiological Sciences
Research Center for Charged Particle Therapy
~from macroscopic to microscopic~
Symposium on Nuclear Data 2004Nov. 12, 2004 @ JAERI, Tokai
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22NIRS / HIMACNIRS / HIMAC
RésuméIntroduction
radiations used for radiotherapywhat to estimate to carry out heavy ion therapy
Macroscopic effectnuclear reaction
dose
Microscopic effectbeam quality
biological effectspatial distribution
advanced irradiationmicrodosimetry
nature of heavy ion radiotherapyneutrons
Summary
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33NIRS / HIMACNIRS / HIMAC
Radiations used for tumor therapy
“Heavy ion”
direct ionizing radiationelectronprotonhelium, carbon, neon, silicon, …:
indirect ionizing radiationphotonneutron:
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44NIRS / HIMACNIRS / HIMACHIMAC (Heavy Ion Medical Accelerator in Chiba)•Established in 1994.•Aimed at finding optimal heavy ion therapy scheme.
0.3 / 0.5 Hzrepetition cycle
100~109 particles/pulsebeam intensity
800 MeV/n(ε=Z/A=1/2)maximum energy
H,He,C,Ne,Si,Ar,Fe,Kr,Xeion species
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55NIRS / HIMACNIRS / HIMAC
Clinical trials at HIMAC• Targets of carbon therapy
brain, scull baseeye head and neck
lung
liver pancreas
prostate, uterus rectum
bone, soft tissue
nasal passagecancer
Nov. 1, 2003: approved as a Highly Advanced Medical Technology¥3.14M / treatment
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66NIRS / HIMACNIRS / HIMAC
Basis of clinical dose prescription
radiation survival
+ ⇒
loss of capacity for
multiplication (inactivation)• cell survival
0.01
0.1
1
0 2 4 6 8 10
Sur
vivi
ng F
ract
ion
Dose (Gy)
reference
test
effectsameradiationtest
radiationreference
DD
RBE __
_=
carbon: 2~3
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77NIRS / HIMACNIRS / HIMAC
Characteristic of heavy-ion therapyFragmentation of incident particles
projectile (carbon)
target
projectile fragmentparticipant
spectator
140-430MeV/n
Projectile fragments have almost
-…same velocity-…same direction
with those of primaries.
Therapeutic beam is
contaminated by fragments!
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88NIRS / HIMACNIRS / HIMAC
Why?
0
1
2
3
4
5
6
0 50 100 150 200
C290 MeV/n in Water
HIBRAGGsmeasurement
Rel
ativ
e D
ose
Depth in Water (mm)
Effect by fragmentationfrom clinical point of view
Production of fragment particles...…causes unwanted dose beyond the range…makes estimation of biological effect complex.…makes it possible to monitor beam range.
M. Scholz et al., Radiat. Environ. Biophys., 36, 59 (1997).T. Nishio (NCC-east), private comm.
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99NIRS / HIMACNIRS / HIMAC
Macroscopic effectDepth dose distribution
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1010NIRS / HIMACNIRS / HIMAC
Depth-dose distributionDose……”quantity of radiation” ][/ GykgJDose =
the most fundamental factor to be controlled on radiotherapy
reaction cross sectionstopping power
multiple scattering and straggling:
physical factors
Disintegration of primariesloss of dominant dose carrier
Production of fragmentsdeliver dose but form ‘fragment tail’ beyond the range
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1111NIRS / HIMACNIRS / HIMAC
Depth-dose distributionDepth-dose distribution in water measured at HIMAC
0
1
2
3
4
5
6
0 50 100 150 200
C290 MeV/n in Water
HIBRACmeasurement
Rel
ativ
e D
ose
Depth in Water (mm)
0
0.5
1
1.5
2
2.5
3
3.5
0 50 100 150 200 250 300 350
C400 MeV/n in Water
HIBRACmeasurement
Rel
ativ
e D
ose
Depth in Water (mm)
Dose can be controlled in clinically enough precision.
basis of ongoing carbon therapy
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1212NIRS / HIMACNIRS / HIMAC
Macroscopic to Microscopic
What? – particle identification
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1313NIRS / HIMACNIRS / HIMAC
Importance of P. I.LET and particle species dependency of RBE (CHO cell)
M. Scholz and G. Kraft, Rad. Prot. Dos., 52, 29 (1994)
How should we take into account this complexity?
Radiation quality (fluence and energy)
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1414NIRS / HIMACNIRS / HIMAC
depth
LET
fragment simulation
How? - NIRS scheme
survival
Biological dataHSG cell
depth
∑= iimix f αα
∑= iimix f ββ
Biol. dose
LQ model:S= exp(-αD-βD2)
dose
dose
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1515NIRS / HIMACNIRS / HIMACHow many? - fluence
12C-290MeV/n Calculation: hibrac (old)
Z=6,2,1 Z=5,4,3
0
0.2
0.4
0.6
0.8
1
0 50 100 150
Z=6Z=2Z=1
Z=6Z=2Z=1
Z=6 (CR39)
Nor
mal
ized
Flu
ence
PMMA Thickness (mm)
0
0.02
0.04
0.06
0.08
0.1
0 50 100 150
Z=5Z=4Z=3
Z=5Z=4Z=3
Z=5 (CR39)Z=4 (CR39)
Nor
mal
ized
Flu
ence
PMMA Thickness (mm)
Need improvement on simulation modelN. Matsufuji et al Phys. Med. Biol., 48, 1605 (2003)
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1616NIRS / HIMACNIRS / HIMACComparison with PHITS
Z=6,2,1 Z=5,4,312C-290MeV/n Calculation: PHITS 1.80
0
0.5
1
1.5
0 20 40 60 80 100 120 140 160
Z=6Z=2Z=1
Z=6Z=2Z=1
Nor
mal
ized
Flu
ence
BF Thickness (mm)
0
0.02
0.04
0.06
0.08
0.1
0 20 40 60 80 100 120 140 160
Z=5Z=4Z=3
Z=5Z=4Z=3
Nor
mal
ized
Flu
ence
BF Thickness (mm)
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1717NIRS / HIMACNIRS / HIMAC
Z=6Z=5Z=4Z=3Z=2Z=1
0
1
2
3
4
5
6
0 50 100 150 200
Rel
ativ
e D
ose
Depth in Water (mm)
102
103
104
101 102
Dos
e (A
rbitr
ary
Uni
t)
LET (keV/µm)
PMMA = 0 mmH2O
102
103
104
101 102
Dos
e (A
rbitr
ary
Uni
t)
LET (keV/µm)
PMMA = 90 mmH2O
102
103
104
101 102
Dos
e (A
rbitr
ary
Uni
t)
LET (keV/µm)
PMMA = 130 mmH2O
LET spectra12C-290MeV/n
100% 81% 77%
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1818NIRS / HIMACNIRS / HIMAC
Heavy-ion therapy sites
LBL NIRSHyogo
GSI
1977~1991
1997~
2002~1994~
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1919NIRS / HIMACNIRS / HIMAC
Where? – spatial distribution
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2020NIRS / HIMACNIRS / HIMAC
Importance of the spatial distributionScanning irradiation with pencil beam
Not fully understood both experimentally / theoretically
(picture from SIEMENS)
lateral nonuniformity
stopping powermultiple scattering
production cross sectionreaction cross sectionmomentum transfer
:
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2121NIRS / HIMACNIRS / HIMAC
More microscopic!- microdosimetric approach
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2222NIRS / HIMACNIRS / HIMAC
Microdosimetric problem• Random energy deposition
in cell nucleus
•amorphous (averaged) track •actual (sparse) track
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2323NIRS / HIMACNIRS / HIMAC
What? – neutrons
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2424NIRS / HIMACNIRS / HIMAC
Neutrons in therapy room12C-290MeV/n 10000 particles (simulation with PHITS)
carbon
neutronscatterer ridge filter collimator patient
Geometry: from Nose (IHI)
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2525NIRS / HIMACNIRS / HIMAC
Neutrons in therapy room12C-290MeV/n 10000 particles (simulation with PHITS)
Neutron dose distribution
scatterer ridge filter collimator patient
•Risk estimation for the induction of the secondary cancer
•Dependency to irradiation scheme
•Optimal treatment method
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2626NIRS / HIMACNIRS / HIMAC
SummaryMacroscopic effect
Charge-changing cross section
Depth-dose distribution is given in good precision
Dose is delivered to tumor accurately
Need further investigation for heavier elements
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2727NIRS / HIMACNIRS / HIMACSummary
Microscopic effectsFluence and LET distribution (broad beam)
Feedback to biology (ex. survival simulation)
Spatial distribution (pencil beam)
Input data for RTP of scanning irradiation
Angular distribution, double differential production cross section, momentum transfer, …
Development of simulation code including spatial information, advanced RTP (inhomogeneous structure)
Microdosimetric approach
Understanding of the nature of heavy ion therapy
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2828NIRS / HIMACNIRS / HIMAC
Thank you for your attention.Thank you for your attention.
Mt. Fuji from Chiba city
A part of this work was carried out as the Research Project with Heavy Ions at HIMAC.